Réka
Mokrai
abc,
Rózsa
Szűcs
ab,
Matthew P.
Duffy
a,
Vincent
Dorcet
a,
Thierry
Roisnel
a,
Zoltán
Benkő
*b,
László
Nyulászi
*bc,
Pierre-Antoine
Bouit
*a and
Muriel
Hissler
*a
aUniv Rennes, CNRS, ISCR - UMR 6226, F-35000 Rennes, France. E-mail: muriel.hissler@univ-rennes1.fr; pierre-antoine.bouit@univ-rennes1.fr
bDepartment of Inorganic and Analytical Chemistry, Budapest University of Technology and Economics Szt. Gellért tér 4 H-1111 Budapest, Hungary. E-mail: zbenko@mail.bme.hu
cMTA-BME Computation Driven Chemistry Research Group. Gellért tér 4 H-1111 Budapest, Hungary. E-mail: nyulaszi@mail.bme.hu
First published on 14th April 2021
Polycyclic Aromatic Hydrocarbons (PAHs) with planar, twisted and negatively curved topologies were obtained from polycyclic phospholes using pericyclic reactions. Deviation from planarity is due to steric interactions between the PAH core and the ester substituents. These structural effects on the optical and redox properties were studied and rationalized through DFT calculations. This synthetic approach thus allows the preparation of topologically diverse PAHs allowing fine-tuning their electronic properties, with potential applications in organic electronics.
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Fig. 1 (a) Representative examples of planar (I), twisted (II) and negatively curved PAHs (III). (b) Synthetic strategy devised in this article. |
The introduction of twist or curvature into the π-conjugated framework affording the so-called contorted PAHs, such as twisted II or negatively Gaussian curved III, (Fig. 1a)2 also appeared as an efficient way to fine-tune their electronic properties. To achieve this, two main strategies are used.3 One is the endo-skeletal approach, in which non-six membered rings are included in polybenzenoid frameworks. The other is the exo-skeletal strategy, whereby one or more cove and/or fjord regions of the fused π-system is contorted by bulky substituents.4 The development of such PAHs is highly challenging since, in the non-planar structure, the stability of the π-system has to be reduced. Thus, the formation of contorted PAHs directly depends on the efficiency of synthetic approaches to control shape, size, curvature and, therefore, to achieve well-tailored properties. In our hypothesis, the energy demand of the distortion of aromaticity can be covered by the use of weakly anti-aromatic λ5,σ4-phosphole derivatives as starting materials.5 The generation of six-membered rings stabilized by aromaticity via cycloaddition-type reactions6 provides the necessary driving force allowing to overcome the energy need of the steric repulsion. We envisage extending this approach to polycyclic phospholes7 to prepare new PAHs, whose structural characteristics will be controlled through the phosphole-based precursor (Fig. 1b). It is worth mentioning that cycloadditions have already been used to prepare PAHs.8 For example, Scott et al. selectively performed cycloadditions on the bay position of perylenes and bisanthenes using diethyl acetylenedicarboxylate.9 Heterocycles such as furanes have also been used to as diene to prepare PAHs.8 However, the rich reactivity of phospholes in cycloaddition prompt us to explore this strategy to prepare novel PAHs.
Herein, we report a selective bottom-up synthesis of topologically diverse PAHs employing pericyclic reactions with polycyclic phospholes and the investigation of their optical and redox properties based on experimental and computational studies.
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Fig. 2 Visualization of the NICS(0) values (B3LYP/6-311 + G*//B3LYP/6-31 + G*) of compounds P, 1, 2 and 6–8. The NICS(0) values (which can be defined unambiguously also in the curved molecules) were presented, nevertheless the NICS(1) values show the same tendencies, see Table S18 (ESI†). |
To extend this approach for achieving structural diversity, we decided to engage a more sterically demanding polyaromatic thioxo-phospholes7 in pericyclic reactions with DMAD (Scheme 2). In similar conditions as for the formation of 2, polycyclic thioxophospholes 3–5, featuring respectively 4, 6 and 8 fused rings,7 were converted into Clar-type benzenoid-based PAHs 6–8 in moderate yields after purification (Scheme 2). These moderate yields come from purification difficulties since the conversion appears quantitative as observed by NMR spectroscopies (see Fig. S8b, ESI†). Following the strategy of Li et al.,13 microwave irradiation was also investigated and afforded better isolated yields in the case of 6. Importantly, all starting phospholes are fully stable in the reaction conditions in absence of dienophile (Fig S8a, ESI†). Again, the phosphanorbornadiene intermediate remained elusive.
However, as an indirect proof for the mechanism, the reaction between 3 and p-benzoquinone as a dienophile resulted in the phosphanorbornene 9 (Scheme 3 and ESI†) because the aromatization is hampered by the two sp3 carbon atoms. The newly formed PAHs can be further functionalized using simple transformations of esters, as exemplified on 6 to afford its bis-imide analogue 10 (Scheme 3 and ESI†). All compounds were unambiguously characterized by multinuclear NMR, HRMS and by X-ray diffraction performed on single crystals (vide infra).
Importantly, the regioselectivity of the pericyclic reactions is exclusively on the dienic system of the P-ring of 1,3–5 and not on the bay position as it has been reported by Scott et al. on various PAHs.9 This clearly emphasizes the role of the P-heterocycle in the regioselectivity. It also unambiguously confirms that the P(S)Ph loss does not occur before the cycloaddition. For 6–8, the replacement of the phosphole ring by a benzenoid unit results in analogous changes as in case of 2, yielding again a Clar aromatic arrangement of the all-fused 8. Significantly, regardless of the distortion from planarity (for the similar NICS pattern of the structures calculated under planarity constraint see ESI†), the aromaticity pattern in these PAHs nicely agrees with Clar's criterion (see the rings marked with white circles in Fig. 2). This observation is further bolstered by the measured bond distances. The bonds of six-membered rings A, C and E are within the typical range of 1.38–1.42 Å, revealing benzenoid character, while in rings B and D the distances between benzenoid rings are significantly longer (1.47–1.48 Å).
Further analysis of the structural data (Fig. 3 and Table S1, ESI†) of 6 and 8 reveals that their polycyclic backbone is highly distorted in both cases in order to accommodate the two ester groups on the central phenyl ring. In addition, different curvatures are observed in these two compounds. Hence, 6 displays a twisted π-backbone with angles between the central ring (in blue, Fig. 3) and the phenyl moiety of the bay-like position (in purple, Fig. 3) of 31.4°. On the contrary, 8 possesses a negative Gaussian curvature (saddle shape) with angles between the methoxy substituted peripheral benzene ring (in green, Fig. 3) and the central ring (in blue, Fig. 3) of 25.9° and 29.4° and angles between the two central rings (blue and red) of 15.1° in the opposite direction. The structure of 7 can also be classified as negatively curved, however the X-ray data did not allow for reliable structural parameter determination (Fig. S11, ESI†). At the intermolecular level, no clear interactions are observed in the crystalline packing of 6, probably because of its highly distorted backbone. However, 8 crystallizes as isolated π-dimers (d = 3.35 Å, Fig. S15, ESI†) by overlapping of the biphenyl moieties indicating that the solid-state structure may be finally determined by the crystal packing effects.
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Fig. 3 Crystallographic structure of 211 (top (a) and side view (b)) 6 (top (c) and side view (d)) and 8 (top (e) and side view (f)). |
To gain insight into the conformational stability of these compounds, we attempted to optimize further conformations from several different starting geometries at the B3LYP/6-31 + G* and B3LYP-D3/6-31 + G* levels. For 6 and 7, only the twisted and negatively curved structures, respectively, were found, which are similar to the ones obtained from the X-ray diffraction. For 8, apart from the negatively curved structure, a twisted isomer was also obtained, and the energy difference between the two conformers is only 0.5 kcal mol−1 (Table S3 and Fig. S32–S33, ESI†). We have also calculated the energy of planarization, by optimizing the PAH part under planarity constraint. For 6, 7 and 8, we have obtained the non-negligible 9.6 kcal mol−1, 10.4 kcal mol−1 and 11.6 kcal mol−1 planarization energies, respectively. Altogether, these data indicate the flexibility of the molecule in the gas phase and likely in solution. Importantly the gas phase structures clearly show significant deviation from planarity, which indicates that the curvature of these molecules is not caused by the crystal packing, but indeed results from the steric repulsion of the substituents.
The analysis of the X-ray structures thus revealed that our synthetic methodology can lead to the formation of planar, twisted or negatively curved PAHs in the solid-state, depending on the nature of the substituents. In precursor 3–5, the five-membered ring with a pyramidal phosphorus atom does not perturb the framework of the sp2-carbon atoms. On the contrary, the introduction of a six-membered ring functionalized with ester groups introduces a torsion of the carbon domain depending on the steric extent of the environment around the bay regions, which had accommodated the phosphorus-centered moiety.
To establish structure–property relationships for these structurally versatile PAHs 2 and 6–8, their UV-vis absorption and fluorescence spectra were recorded in DCM (Fig. 4) at room temperature and their cyclic voltammetry was measured in DCM using Bu4NPF6 as the electrolyte (Table 1). Furthermore, TD-DFT calculations were performed at the B3LYP/6-31 + G* level of theory. The replacement of the phosphole ring, known to have a stabilized LUMO level, by a benzenoid unit strongly influences the redox properties. While the oxidation potentials remain almost unchanged for 1 and 2, the reduction potential decreases significantly for 2, characteristic of the formation of the Clar aromatic pattern. 6 displays irreversible oxidation and reduction processes (Table 1) at rather high potentials. The extension of the π-systems in the series 6–8 leads to a decrease of the oxidation potentials and an increase of the reduction potentials (Table 1). The stability of the reduced and oxidized forms also increases since the redox potentials of 8 become reversible. Accordingly, the LUMO and HOMO levels decrease and increase, respectively (Table 1).
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Fig. 4 UV-vis absorption (top) and emission (down) of 2 (yellow), 6 (blue), 7 (red) and 8 (green) in diluted DCM. (all compounds are excited at λmax except 2 (λexc = 386 nm)). |
λ abs (nm) | log ε | λ em (nm) | Φb % | E ox (V) | E red (V) | HOMOe (eV) | LUMOe (eV) | |
---|---|---|---|---|---|---|---|---|
a In CH2Cl2 (10−5M). Calculated values shown in parentheses (TD-B3LYP/6-31+G*). b Measured relative to quinine sulfate (H2SO4, 0.1 M), ϕ = 55%. c In CH2Cl2 with Bu4N+PF6− (0.2 M) at a scan rate of 100 mVs−1. Eox(Ered) = Epc (Epa). Potentials vs ferrocene/ferrocenium. d Quasi-reversible processes. e At the B3LYP/6-31 + G* level. f Negatively curved structure. g Twisted structure. | ||||||||
1 | 486 | 4.2 | 509 | 69 | +0.83d | −1.80d | −5.53 | −2.66 |
(424) | (575) | |||||||
2 11 | 386, 424 | 4.1, 3.3 | 463 | 64 | +0.87d | −2.25d | −5.65 | −2.19 |
6 | 277 | 4.3 | 411 | <1% | +1.15 | −2.38 | −5.98 | −1.68 |
(310) | (472) | |||||||
7 | 325, 374 | 4.5, 3.9 | 496 | 6 | +0.85 | −2.28 | −5.62 | −1.85 |
(334, 378) | (602) | |||||||
8 | 341, 385 | 4.3, 3.7 | 505 | 15 | +0.67 | −2.04d | −5.41f | −1.96f |
(347, 415)e | (521)f | −5.43g | −1.78g | |||||
(345, 399)f | (426)g |
The absorption spectrum of the planar phosphole-based PAH 1 shows structured transitions (λabsmax = 486 nm) belonging to the HOMO → LUMO π–π* transition and corresponding to vibrational fine structures characteristic of polyaromatic molecules (Fig. S35, ESI†). In DCM, 1 shows intense and structured emission which is nearly the perfect mirror image of the absorption spectrum with a respective maximum at 509 nm (Fig. S16, ESI†). The insertion of the six–membered ring in place of the phosphole ring resulting in 2, induces a blue shift of the absorption bands. The spectrum itself, (as previously described)11 is dominated by a 386 nm structured band, accompanied by a low-intensity band centered at 424 nm. Both ADC(2) and TD-B3LYP calculations reproduce this intensity pattern. According to the TD-DFT calculations, the 424 nm (λcalc= 398 nm) band belongs mainly to the HOMO → LUMO+1 transition, while the more intense band at 386 nm (λcalc= 392 nm) is the HOMO → LUMO transition. Both bands are mainly π–π* transitions since HOMO, LUMO and LUMO+1 are localized at the planar PAH framework. However, LUMO+1 has a significant contribution of the rather floppy ester functionalities (Fig. S26, ESI†) leading to the presence of the vibronic structure only at the 386 nm band.
6–8 also exhibit significantly blue-shifted absorption bands compared to their phosphole precursors, which are in agreement with the increasing aromaticity upon replacement of the phosphorus-based unit by a CC fragment. Furthermore, no vibrational fine structures in the absorption bands characteristic for planar PAH appear for 6–8 exhibiting contorted backbone (Fig. 4). The absorption spectra of the PAHs 6, 7 and 8 show a gradual bathochromic shift in the series in accordance with the increase in π-conjugation and the above discussed variation of their FMO energies. Furthermore, TD-DFT calculations (Tables S8, S10 and S12, ESI†) show that the tailing features of these spectra can be explained by low energy transitions of rather low intensity (two excitations for 6 and three for 7 and 8). In all these transitions, several electron configurations are mixed (Tables S8, S10 and S12), but the HOMO → LUMO being the main contributor for the first excitations of 7 and 8. The curvature of the molecules and the presence of flexible substituents lead to the lack of vibronic structures. Furthermore, in case of 8, the possible contribution from the twisted form in the solution acts also broadening.
All these compounds (1, 2, 6–8) are fluorescent in solution. A bathochromic shift of emission wavelengths is observed in the series 6–8, together with an increase in the fluorescence quantum yield. The low fluorescence quantum yield of 6 is in accordance with the low oscillator strength of the absorption and the flexibility of the molecule. Although their quantum yield does not reach the high value of the perfectly planar 2,11 going from the poorly luminescent 6 to the good fluorophore 8, the rigidity of their structure increases alongside with their quantum yield.
Reactions under microwave irradiations were realized in the Anton Paar Monowave 300® microwave reactor (Anton Paar France) of the S2 Wave platform, ScanMAT UMS CNRS 2001, Rennes. Microwave irradiation reactions were realized in borosilicate glass vials of 10 ml equipped with snap caps (at the end of the irradiation, cooling reaction was realized by compressed air) with the Monowave® 300 reactor. The microwave instrument consists of a continuous focused microwave power output from 0 to 800W for the Anton Paar Monowave 300® apparatus. All the experiments in this microwave reactor were performed using stirring option. The target temperature was reached with a ramp of 2–5 minutes and the chosen microwave power stayed constant to hold the mixture at this temperature. The reaction temperature was monitored using calibrated infrared sensor and the reaction time included the ramp period. The microwave irradiation parameters (power and temperature) were monitored by the internal software package for the Monowave® 300 Anton–Paar. All the other reactions were, carried out in closed Schlenk and the temperature indicated were measured inside the oil bath.
1H, 13C, and 31P NMR spectra were recorded on Bruker AV III 400 MHz NMR and 300 MHz spectrometers equiped with BBO or BBFO probeheads. Assignment of proton and carbon atoms is based on COSY, NOESY, edited-HSQC and HMBC experiments. 1H and 13C NMR chemical shifts were reported in parts per million (ppm) using residual solvent signal as reference. High-resolution mass spectra were obtained on a Varian MAT 311 or ZabSpec TOF Micromass instrument at Scanmat-UMS 2001, University of Rennes 1 and Maxis 4G. Elemental analyses were performed by Scanmat-UMS 2001, University of Rennes 1. Compounds 2–5 and 7-phenyldinaphtho[2,1-6:
1′,2′-d]oxophosphole were synthesized according to published procedures.7,10 UV-Visible spectra were recorded at room temperature on a JASCO V-630 spectrophotometer. The UV-vis-NIR emission and excitation spectra measurements were recorded on a FL 920 Edimburgh Instrument equipped with a Hamamatsu R5509-73 photomultiplier for the NIR domain (300–1700 nm) and corrected for the response of the photomultiplier. Quantum yields were calculated relative to quinine sulfate (ϕ = 0.55 in H2SO4 0.1M). The electrochemical studies were carried out under argon using an Eco Chemie Autolab PGSTAT 30 potentiostat for cyclic voltammetry with the three-electrode configuration: the working electrode was a platinum disk, the reference electrode was a saturated calomel electrode and the counter-electrode was a platinum wire. All potentials were internally referenced to the ferrocene/ferrocenium couple. For the measurements, concentrations of 10−3 M of the electroactive species were used in freshly distilled and degassed dichloromethane and 0.2 M tetrabutylammonium hexafluorophosphate.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1973069, 1895041, 1956170, 1895043, 1895042 and 1973065. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1nj01194d |
This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2021 |